dorsal/arxiv
View SchemaSuperconductivity from correlated hopping
| Authors | C. D. Batista, F. Lema, A. A. Aligia |
|---|---|
| Categories | |
| ArXiv ID | supr-con/9505001 |
| URL | https://arxiv.org/abs/supr-con/9505001 |
| DOI | 10.1103/PhysRevB.52.6223 |
Abstract
We consider a chain described by a next-nearest-neighbor hopping combined with a nearest-neighbor spin flip. In two dimensions this three-body term arises from a mapping of the three-band Hubbard model for CuO$_2$ planes to a generalized $t-J$ model and for large O-O hopping favors resonance-valence-bond superconductivity of predominantly $d$-wave symmetry. Solving the ground state and low-energy excitations by analytical and numerical methods we find that the chain is a Luther-Emery liquid with correlation exponent $K_{\rho} = (2-n)^2/2$, where $n$ is the particle density.
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"date_modified": "2026-03-02T18:02:51.615000Z",
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"abstract": "We consider a chain described by a next-nearest-neighbor hopping combined\nwith a nearest-neighbor spin flip. In two dimensions this three-body term\narises from a mapping of the three-band Hubbard model for CuO$_2$ planes to a\ngeneralized $t-J$ model and for large O-O hopping favors resonance-valence-bond\nsuperconductivity of predominantly $d$-wave symmetry. Solving the ground state\nand low-energy excitations by analytical and numerical methods we find that the\nchain is a Luther-Emery liquid with correlation exponent $K_{\\rho} =\n(2-n)^2/2$, where $n$ is the particle density.",
"arxiv_id": "supr-con/9505001",
"authors": [
"C. D. Batista",
"F. Lema",
"A. A. Aligia"
],
"categories": [
"supr-con",
"cond-mat.supr-con"
],
"doi": "10.1103/PhysRevB.52.6223",
"title": "Superconductivity from correlated hopping",
"url": "https://arxiv.org/abs/supr-con/9505001"
},
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